The magnetic charge carried by each pole of the Nambu MAP is a fraction, \(\pm \frac{4\pi }{e}\sin ^2\theta _{\scalebox {.5}{\mbox{W}}}\) . In contrast, the poles of Cho-Maison MAP in this paper carry non-fractional magnetic charge of \(\pm \frac{4\pi }{e}\) . The MAP configuration was investigated at physical Weinberg angle, \(\tan \theta _{\scalebox {.5}{\mbox{W}}}=0.53557042\) , while the Higgs self-coupling constant, \(\beta \) , runs from 0 to 1.7704 and at physical \(\beta =0.77818833\) , while \(\tan \theta _{\scalebox {.5}{\mbox{W}}}\)  is allowed to vary (\(0.4675\le \tan \theta _{\scalebox {.5}{\mbox{W}}}\le 10\) ). For better comparison, numerical solutions found in the SU(2)\(\times \) U(1) WS theory were compared with MAP solutions of Kleihaus and Kunz [1]} when \(\phi \) -winding number, \(n=1\) . The investigated quantities include magnetic dipole moment (\(\mu _m\) ), pole separation (\(d_z\) ) and the Higgs modulus at the origin (\(z_0\) ).
